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(7.10)

j dpdq [U - Jft'(p, q)] e{3[A(V,T)-.Yf'(p,q ) = 0

Sequence diagrams allow you to convey some information, for example, timing information, which cannot be conveyed via collaboration diagrams Collaboration diagrams also tend to become difficult to comprehend once you exceed a few objects on the diagram, whereas sequence diagrams have proven to be capable of handling scenarios involving a large number of objects

(7.11)

+ jdpdqe{3(A-.Yf') (U _ Jft')(A _ Jft'-

(7.12)

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The preceding caveats aside, for all practical purposes, the distinction is really one of preference It is relatively straightforward to derive a sequence diagram from a collaboration diagram and vice versa

By (7.8) this can be rewritten in the form au a/3 + ((U - Jft')2)

(7.13)

(Jft'2) - (Jft')2

Figure 8- 8

(7.14)

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For a macroscopic system (Jft') 0:: Nand C v 0:: N. Hence (7.14) is a normal fluctuation. As N --+ 00, almost all systems in the ensemble have the energy (Jft'), which is the internal energy. Therefore the canonical ensemble is equivalent to the microcanonical ensemble. It is instructive to calculate the fluctuations in another way. We begin by calculating the partition function in the following manner:

1 dEw(E) e-{3E = 1 dEe-{3E+!ogw(E)

Figure 8 - 7

00 00

faoo dE e{3[TS(E)-E)

(7.15)

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